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Unitary representations correspond to nondegenerate star representations of L one

Statement

Assume the Axiom of Choice. Let G be an LCH group. The assignment π↦σπ, σπ(f):=π(f), from strongly continuous unitary representations of G to star-representations of the Banach ∗-algebra L1(G) (Strongly continuous unitary representations, invariant linear subspaces and intertwiners, The integrated form of a unitary representation, Nondegenerate star-representations of a Banach star-algebra) is a bijection, respecting unitary equivalence, between unitary representations of G up to unitary equivalence and nondegenerate star-representations of L1(G) up to equivalence: every unitary representation has a nondegenerate integrated form, every nondegenerate star-representation is the integrated form of a unique unitary representation, and a unitary intertwines two representations if and only if it intertwines their integrated forms.

Facts & Assumptions

Given: AC; an LCH group G; strongly continuous unitary representations of G; nondegenerate star-representations of L1(G).

[F1]

The integrated form f↦π(f) of a unitary representation is a contractive nondegenerate star-representation of L1(G), and π(f)ξ is characterised by ⟨π(f)ξ,η⟩=∫Gf(g)⟨π(g)ξ,η⟩ dg (Integrated forms are contractive nondegenerate star representations of L one, The integrated form of a unitary representation).

[F2]

Conversely, every nondegenerate star-representation σ of L1(G) on a Hilbert space K is the integrated form of a unique unitary representation U of G; it satisfies U(g)σ(f)ξ=σ(Lgf)ξ for all g,f,ξ (Recovering a unitary group representation from a nondegenerate L one representation).

[F3]

L1(G) has a two-sided approximate unit (eU) with ∥eU∥1≤1, eU∗f→f, f∗eU→f (L1 group algebras have a contractively bounded approximate identity).

[F4]

Lgf(x)=f(g−1x) defines an isometric linear map of L1(G) with Lg(a∗b)=(Lga)∗b and LgLh=Lgh (Recovering a unitary group representation from a nondegenerate L one representation); moreover π(LgeU)ξ→π(g)ξ for every unitary representation π and every ξ, because left invariance gives π(LgeU)ξ=∫GeU(y)π(gy)ξ dy and eU≥0 has total mass one and support shrinking to {e}, so the norm difference is at most sup⁡y∈U∥π(gy)ξ−π(g)ξ∥. [F1, F3]

Proof

technique · direct

Given: AC, an LCH group G, and the integrated-form assignment π↦σπ.

1.1F1F2F4

The assignment is well defined on equivalence classes and preserves equivalence: by [F1] each σπ is a nondegenerate star-representation; and if U:Hπ→Hρ is a unitary intertwiner, Uπ(g)=ρ(g)U, then the defining weak integrals give Uσπ(f)=σρ(f)U for every f∈L1(G), since U passes through the integral. Conversely, if U intertwines the integrated forms, it intertwines each π(LgeV) with ρ(LgeV); their strong limits are π(g) and ρ(g) by [F4], so Uπ(g)=ρ(g)U. Thus a specified unitary intertwines the group representations exactly when it intertwines their integrated forms.

1.2F1F3F4

For every unitary representation π, every g∈G, f∈L1(G) and ξ∈Hπ: π(g)π(f)ξ=π(Lgf)ξ. Indeed, Lg(eU∗f)=(LgeU)∗f by [F4], so π(Lg(eU∗f))=π(LgeU)π(f) by multiplicativity [F1]; as Lg(eU∗f)→Lgf in L1(G) and π(LgeU)→π(g) strongly by [F4], both sides converge to π(Lgf)ξ and π(g)π(f)ξ respectively.

1.3F2

Surjectivity: given a nondegenerate star-representation σ, [F2] produces a unitary representation U with πU(f)=σ(f) for all f, so every nondegenerate star-representation is an integrated form.

2.1F2step 1.2

Injectivity: suppose unitary representations π and π′ have the same integrated form σ. By [F2] applied to σ there is a unique unitary representation U with U(g)σ(f)ξ=σ(Lgf)ξ; by step 1.2 both π and π′ satisfy this identity, because σ(f)=π(f)=π′(f); hence π=U=π′. Thus the assignment is injective on equivalence classes.

3.1F1F2step 1.1step 1.3step 2.1∎

Combining steps 1.1, 1.3 and 2.1, the assignment induces a bijection between unitary equivalence classes of unitary representations and equivalence classes of nondegenerate star-representations, and step 1.1 shows exactly that it respects unitary equivalence in both directions. The Axiom of Choice is carried by the integrated-form correspondence of [F1]–[F2] as declared throughout this page (The Axiom of Choice).

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